《时间简史―从大爆炸到黑洞》 ――史蒂芬?霍金

Newton realized that, according to his theory of gravity, the stars should attract each other, so it seemed they could not remain essentially motionless. Would they not all fall together at some point? In a letter in 1691 to Richard Bentley, another leading thinker of his day, Newton argued that this would indeed happen if there were only a finite number of stars distributed over a finite region of space. But he reasoned that if, on the other hand, there were an infinite number of stars, distributed more or less uniformly over infinite space, this would not happen, because there would not be any central point for them to fall to.
    This argument is an instance of the pitfalls that you can encounter in talking about infinity. In an infinite universe, every point can be regarded as the center, because every point has an infinite number of stars on each side of it. The correct approach, it was realized only much later, is to consider the finite situation, in which the stars all fall in on each other, and then to ask how things change if one adds more stars roughly uniformly distributed outside this region. According to Newton’s law, the extra stars would make no difference at all to the original ones on average, so the stars would fall in just as fast. We can add as many stars as we like, but they will still always collapse in on themselves. We now know it is impossible to have an infinite static model of the universe in which gravity is always attractive.
    It is an interesting reflection on the general climate of thought before the twentieth century that no one had suggested that the universe was expanding or contracting. It was generally accepted that either the universe had existed forever in an unchanging state, or that it had been created at a finite time in the past more or less as we observe it today. In part this may have been due to people’s tendency to believe in eternal truths, as well as the comfort they found in the thought that even though they may grow old and die, the universe is eternal and unchanging.
    Even those who realized that Newton’s theory of gravity showed that the universe could not be static did not think to suggest that it might be expanding. Instead, they attempted to modify the theory by making the

A Brief History of Time - Stephen Hawking... Chapter 1
gravitational force repulsive at very large distances. This did not significantly affect their predictions of the
motions of the planets, but it allowed an infinite distribution of stars to remain in equilibrium

Aristotle, and most of the other Greek philosophers, on the other hand, did not like the idea of a creation
because it smacked too much of divine intervention. They believed, therefore, that the human race and the
world around it had existed, and would exist, forever. The ancients had already considered the argument about
progress described above, and answered it by saying that there had been periodic floods or other disasters that
repeatedly set the human race right back to the beginning of civilization.
The questions of whether the universe had a beginning in time and whether it is limited in space were later
extensively examined by the philosopher Immanuel Kant in his monumental (and very obscure) work Critique of
Pure Reason, published in 1781. He called these questions antinomies (that is, contradictions) of pure reason
because he felt that there were equally compelling arguments for believing the thesis, that the universe had a
beginning, and the antithesis, that it had existed forever. His argument for the thesis was that if the universe did
not have a beginning, there would be an infinite period of time before any event, which he considered absurd.
The argument for the antithesis was that if the universe had a beginning, there would be an infinite period of
time before it, so why should the universe begin at any one particular time? In fact, his cases for both the thesis
and the antithesis are really the same argument. They are both based on his unspoken assumption that time
continues back forever, whether or not the universe had existed forever. As we shall see, the concept of time
has no meaning before the beginning of the universe. This was first pointed out by St. Augustine. When asked:
“What did God do before he created the universe?” Augustine didn’t reply: “He was preparing Hell for people
who asked such questions.” Instead, he said that time was a property of the universe that God created, and
that time did not exist before the beginning of the universe.
When most people believed in an essentially static and unchanging universe, the question of whether or not it
had a beginning was really one of metaphysics or theology. One could account for what was observed equally
well on the theory that the universe had existed forever or on the theory that it was set in motion at some finite

A Brief History of Time - Stephen Hawking... Chapter 1
time in such a manner as to look as though it had existed forever. But in 1929, Edwin Hubble made the
landmark observation that wherever you look, distant galaxies are moving rapidly away from us. In other words,
the universe is expanding. This means that at earlier times objects would have been closer together. In fact, it
seemed that there was a time, about ten or twenty thousand million years ago, when they were all at exactly
the same place and when, therefore, the density of the universe was infinite. This discovery finally brought the
question of the beginning of the universe into the realm of science.
Hubble’s observations suggested that there was a time, called the big bang, when the universe was
infinitesimally small and infinitely dense. Under such conditions all the laws of science, and therefore all ability
to predict the future, would break down. If there were events earlier than this time, then they could not affect
what happens at the present time. Their existence can be ignored because it would have no observational
consequences. One may say that time had a beginning at the big bang, in the sense that earlier times simply
would not be defined. It should be emphasized that this beginning in time is very different from those that had
been considered previously. In an unchanging universe a beginning in time is something that has to be
imposed by some being outside the universe; there is no physical necessity for a beginning. One can imagine
that God created the universe at literally any time in the past. On the other hand, if the universe is expanding,
there may be physical reasons why there had to be a beginning. One could still imagine that God created the
universe at the instant of the big bang, or even afterwards in just such a way as to make it look as though there
had been a big bang, but it would be meaningless to suppose that it was created before the big bang. An
expanding universe does not preclude a creator, but it does place limits on when he might have carried out his
job!
In order to talk about the nature of the universe and to discuss questions such as whether it has a beginning or
an end, you have to be clear about what a scientific theory is. I shall take the simpleminded view that a theory
is just a model of the universe, or a restricted part of it, and a set of rules that relate quantities in the model to
observations that we make. It exists only in our minds and does not have any other reality (whatever that might
mean). A theory is a good theory if it satisfies two requirements. It must accurately describe a large class of
observations on the basis of a model that contains only a few arbitrary elements, and it must make definite
predictions about the results of future observations. For example, Aristotle believed Empedocles’s theory that
everything was made out of four elements, earth, air, fire, and water. This was simple enough, but did not make
any definite predictions. On the other hand, Newton’s theory of gravity was based on an even simpler model, in
which bodies attracted each other with a force that was proportional to a quantity called their mass and
inversely proportional to the square of the distance between them. Yet it predicts the motions of the sun, the
moon, and the planets to a high degree of accuracy.

Any physical theory is always provisional, in the sense that it is only a hypothesis: you can never prove it. No
matter how many times the results of experiments agree with some theory, you can never be sure that the next
time the result will not contradict the theory. On the other hand, you can disprove a theory by finding even a
single observation that disagrees with the predictions of the theory. As philosopher of science Karl Popper has
emphasized, a good theory is characterized by the fact that it makes a number of predictions that could in
principle be disproved or falsified by observation. Each time new experiments are observed to agree with the
predictions the theory survives, and our confidence in it is increased; but if ever a new observation is found to
disagree, we have to abandon or modify the theory.
At least that is what is supposed to happen, but you can always question the competence of the person who
carried out the observation.
In practice, what often happens is that a new theory is devised that is really an extension of the previous theory.
For example, very accurate observations of the planet Mercury revealed a small difference between its motion
and the predictions of Newton’s theory of gravity. Einstein’s general theory of relativity predicted a slightly
different motion from Newton’s theory. The fact that Einstein’s predictions matched what was seen, while
Newton’s did not, was one of the crucial confirmations of the new theory. However, we still use Newton’s theory
for all practical purposes because the difference between its predictions and those of general relativity is very
small in the situations that we normally deal with. (Newton’s theory also has the great advantage that it is much
simpler to work with than Einstein’s!)
The eventual goal of science is to provide a single theory that describes the whole universe. However, the

A Brief History of Time - Stephen Hawking... Chapter 1
approach most scientists actually follow is to separate the problem into two parts. First, there are the laws that
tell us how the universe changes with time. (If we know what the universe is like at any one time, these physical
laws tell us how it will look at any later time.) Second, there is the question of the initial state of the universe.
Some people feel that science should be concerned with only the first part; they regard the question of the
initial situation as a matter for metaphysics or religion. They would say that God, being omnipotent, could have
started the universe off any way he wanted. That may be so, but in that case he also could have made it
develop in a completely arbitrary way. Yet it appears that he chose to make it evolve in a very regular way
according to certain laws. It therefore seems equally reasonable to suppose that there are also laws governing
the initial state.
It turns out to be very difficult to devise a theory to describe the universe all in one go. Instead, we break the
problem up into bits and invent a number of partial theories. Each of these partial theories describes and
predicts a certain limited class of observations, neglecting the effects of other quantities, or representing them
by simple sets of numbers. It may be that this approach is completely wrong. If everything in the universe
depends on everything else in a fundamental way, it might be impossible to get close to a full solution by
investigating parts of the problem in isolation. Nevertheless, it is certainly the way that we have made progress
in the past. The classic example again is the Newtonian theory of gravity, which tells us that the gravitational
force between two bodies depends only on one number associated with each body, its mass, but is otherwise
independent of what the bodies are made of. Thus one does not need to have a theory of the structure and
constitution of the sun and the planets in order to calculate their orbits.
Today scientists describe the universe in terms of two basic partial theories

Now, if you believe that the universe is not arbitrary, but is governed by definite laws, you ultimately have to
combine the partial theories into a complete unified theory that will describe everything in the universe. But
there is a fundamental paradox in the search for such a complete unified theory. The ideas about scientific
theories outlined above assume we are rational beings who are free to observe the universe as we want and to
draw logical deductions from what we see.
In such a scheme it is reasonable to suppose that we might progress ever closer toward the laws that govern
our universe. Yet if there really is a complete unified theory, it would also presumably determine our actions.
And so the theory itself would determine the outcome of our search for it! And why should it determine that we
come to the right conclusions from the evidence? Might it not equally well determine that we draw the wrong
conclusion.? Or no conclusion at all?
The only answer that I can give to this problem is based on Darwin’s principle of natural selection. The idea is
that in any population of self-reproducing organisms, there will be variations in the genetic material and
upbringing that different individuals have. These differences will mean that some individuals are better able
than others to draw the right conclusions about the world around them and to act accordingly. These individuals
will be more likely to survive and reproduce and so their pattern of behavior and thought will come to dominate.
It has certainly been true in the past that what we call intelligence and scientific discovery have conveyed a
survival advantage. It is not so clear that this is still the case: our scientific discoveries may well destroy us all,
and even if they don’t, a complete unified theory may not make much difference to our chances of survival.
However, provided the universe has evolved in a regular way, we might expect that the reasoning abilities that
natural selection has given us would be valid also in our search for a complete unified theory, and so would not
lead us to the wrong conclusions.

Because the partial theories that we already have are sufficient to make accurate predictions in all but the most
extreme situations, the search for the ultimate theory of the universe seems difficult to justify on practical
grounds. (It is worth noting, though, that similar arguments could have been used against both relativity and
quantum mechanics, and these theories have given us both nuclear energy and the microelectronics
revolution!) The discovery of a complete unified theory, therefore, may not aid the survival of our species. It
may not even affect our lifestyle. But ever since the dawn of civilization, people have not been content to see
events as unconnected and inexplicable. They have craved an understanding of the underlying order in the
world. Today we still yearn to know why we are here and where we came from. Humanity’s deepest desire for
knowledge is justification enough for our continuing quest. And our goal is nothing less than a complete
description of the universe we live in.

A Brief History of Time - Stephen Hawking... Chapter 2
CHAPTER 2
SPACE AND TIME
Our present ideas about the motion of bodies date back to Galileo and Newton. Before them people believed
Aristotle, who said that the natural state of a body was to be at rest and that it moved only if driven by a force or
impulse. It followed that a heavy body should fall faster than a light one, because it would have a greater pull
toward the earth.
The Aristotelian tradition also held that one could work out all the laws that govern the universe by pure
thought: it was not necessary to check by observation. So no one until Galileo bothered to see whether bodies
of different weight did in fact fall at different speeds. It is said that Galileo demonstrated that Aristotle’s belief
was false by dropping weights from the leaning tower of Pisa. The story is almost certainly untrue, but Galileo
did do something equivalent: he rolled balls of different weights down a smooth slope. The situation is similar to
that of heavy bodies falling vertically, but it is easier to observe because the Speeds are smaller. Galileo’s
measurements indicated that each body increased its speed at the same rate, no matter what its weight. For
example, if you let go of a ball on a slope that drops by one meter for every ten meters you go along, the ball
will be traveling down the slope at a speed of about one meter per second after one second, two meters per
second after two seconds, and so on, however heavy the ball. Of course a lead weight would fall faster than a
feather, but that is only because a feather is slowed down by air resistance. If one drops two bodies that don’t
have much air resistance, such as two different lead weights, they fall at the same rate. On the moon, where
there is no air to slow things down, the astronaut David R. Scott performed the feather and lead weight
experiment and found that indeed they did hit the ground at the same time.
Galileo’s measurements were used by Newton as the basis of his laws of motion. In Galileo’s experiments, as a
body rolled down the slope it was always acted on by the same force (its weight), and the effect was to make it
constantly speed up. This showed that the real effect of a force is always to change the speed of a body, rather
than just to set it moving, as was previously thought. It also meant that whenever a body is not acted on by any
force, it will keep on moving in a straight line at the same speed. This idea was first stated explicitly in Newton’s
Principia Mathematica, published in 1687, and is known as Newton’s first law. What happens to a body when a
force does act on it is given by Newton’s second law. This states that the body will accelerate, or change its
speed, at a rate that is proportional to the force. (For example, the acceleration is twice as great if the force is
twice as great.) The acceleration is also smaller the greater the mass (or quantity of matter) of the body. (The
same force acting on a body of twice the mass will produce half the acceleration.) A familiar example is

provided by a car: the more powerful the engine, the greater the acceleration, but the heavier the car, the
smaller the acceleration for the same engine. In addition to his laws of motion, Newton discovered a law to
describe the force of gravity, which states that every body attracts every other body with a force that is
proportional to the mass of each body. Thus the force between two bodies would be twice as strong if one of
the bodies (say, body A) had its mass doubled. This is what you might expect because one could think of the
new body A as being made of two bodies with the original mass. Each would attract body B with the original
force. Thus the total force between A and B would be twice the original force. And if, say, one of the bodies had
twice the mass, and the other had three times the mass, then the force would be six times as strong. One can
now see why all bodies fall at the same rate: a body of twice the weight will have twice the force of gravity
pulling it down, but it will also have twice the mass. According to Newton’s second law, these two effects will
exactly cancel each other, so the acceleration will be the same in all cases.
Newton’s law of gravity also tells us that the farther apart the bodies, the smaller the force. Newton’s law of
gravity says that the gravitational attraction of a star is exactly one quarter that of a similar star at half the
distance. This law predicts the orbits of the earth, the moon, and the planets with great accuracy. If the law
were that the gravitational attraction of a star went down faster or increased more rapidly with distance, the
orbits of the planets would not be elliptical, they would either spiral in to the sun or escape from the sun.
The big difference between the ideas of Aristotle and those of Galileo and Newton is that Aristotle believed in a
preferred state of rest, which any body would take up if it were not driven by some force Or impulse. In
particular, he thought that the earth was at rest. But it follows from Newton’s laws that there is no unique